Frequency Spectra Analysis of Drawbar Pulls Generated by Special Driving Wheels Improving Tractive Performance
Abstract
:1. Introduction
2. Materials and Methods
2.1. Design of Driving Wheels
2.2. Drawbar Pull Measurement System
- The test tractor MT8-070 Mini (Agrozet, a. s., Prostějov, Czech Republic) with a gasoline engine with the volume capacity of 400 cm3, rated engine power of 8 kW, and rated engine speed of 3600 min−1 pulling the load tractor to generate the drawbar pull. Three types of driving wheels (the standard tires, the blade wheels, and the spike tires) were mounted to the test tractor. The curb weight of the test tractor was 310 kg. The driver weight was 90 kg. The weight distribution on axes of the test tractor was published by [27].
- The load tractor 4K-14 (Agrozet, a. s., Prostějov, Czech Republic) with a diesel engine with the volume capacity of 661.6 cm3, maximum output power of 13 kW loading the test tractor during the measurement of drawbar pull. The curb weight of the load tractor was 870 kg. The driver weight was 80 kg.
- The load cell EMS 150 (Emsyst, s. r. o., Trenčín, Slovak Republic) with a strain-gauge bridge in steel housing (with accuracy of 0.2% or ±20 N, rated capacity: 10 kN). Output signal (sensitivity of strain-gauge) was 2 mV/V. It means that the output signal in mV obtained at the nominal loading depends on the voltage supply of the strain-gauge in V. At the recommended supply 10 V and nominal loading 10 kN, the output signal was 20 mV. The uncertainty of the measurement was ±2 mV or ±20 N. The data logger HMG 3010 (Hydac GmbH, Sulzbach, Germany) is a high-performance portable measuring and data-logging device [28,29] with accuracy ≤0.1%. The sampling frequency was set to 1 kHz. Resolution was 12 bit. The sensitivity of the measurement range from 0 to 10 V was 10/4096, i.e., 2.4 mV/bit. The uncertainty of the measurement was ±2.4 mV. The total uncertainty of the measurement was ±4.4 mV or ±44 N.
- The power supply contains two accumulators (12 V) connected in series or parallel to supply the sensor and data logger with direct voltage (12 V or 24 V). The power supply was manufactured as a portable device.
- The measurement of drawbar pull was performed at the distance of 30 m. The time of one passage from the start to the end was measured by a stopwatch to determine the test tractor velocity, as shown in Figure 4. The tractor with each driving wheel type did not move in the driving tracts after previous measurements. The tests have never been repeated on the previous tracks. The grass plot was large enough to move the tractor into a new place for each measurement.
- A wheel gauge of the test and load tractor was 0.65 m and 0.85 m. Considering the increase in the wheel gauge of the test tractor with the blade wheel and tire width of both tractors, the load tractor moved on the grass plot surface, but was yes, the change retains the meaning partially disrupted by the special driving wheels. To eliminate the influence of the grass plot surface conditions on the breaking forces, the four-wheel drive load tractor with an adequate weight was used. The weight of the load tractor was more than two times higher than the test tractor.
- Soil properties affect the force interaction between the ground and wheels. The drawbar pull of the tractor with different types of driving wheels was measured at the same soil type of the grass plot and at the same soil moisture to eliminate the change of measured values due to soil properties. The total weight of the tractor is the main parameter that affects the drawbar pull. When the standard and spike tires were used, the rims of driving wheels were ballasted with the correct additional weight to reach the same tractor weight as in the case of the blade wheels. The drawbar pull measurements were performed in accordance with [30]. The test tractor was in the second gear (gear ratio i2 = 146.3) and operated at the rated rotation speed of the engine (3600 min−1).
2.3. FFT Analysis of Drawbar Pull Signals
- X[m] = M-th value of the sequence from the frequency domain (the whole sequence is also referred to as the spectrum);
- x[n] = N-th sample of the time sequence;
- m = Order of the output sample;
- n = Order of the input sample;
- N = Total number of input samples.
- L = length(X);
- n = 2^nextpow2(L);
- Y = fft(X,n)/L;
- f = Fs/2*linspace(0,1,n/2+1);
- y = 2*abs(Y(1:NFFT/2+1));
- plot(f, y);
- XRMS = RMS value;
- x[n] = Nth sample of the time sequence;
- N = Total number of input samples.
2.4. Parameters Describing the Special Driving Wheel Properties
- L = Distance of grass plot (30 m), in m;
- T—Time, in s.
- v = Tractor speed, in m s−1;
- FD = Mean drawbar pull, in N.
- ne = Actual engine speed, in s−1;
- i2 = Gear ratio.
- 16 elements of tire tread pattern of standard tire (rubber lugs);
- 10 elements of blade wheel;
- 4 elements of spike tire.
- E = Number of elements of one driving wheel;
- nw = Rotation speed of driving wheels, in s−1.
2.5. Experimental Conditions
3. Results and Discussion
3.1. Properties and Application of Special Driving Wheels
3.2. Evaluation of Drawbar Pull Frequency Spectra
4. Conclusions
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Acknowledgments
Conflicts of Interest
References
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Parameter | Unit | Value |
---|---|---|
gravel | % | 15.3 |
sand | % | 45.2 |
silt | % | 35.4 |
clay | % | 4.1 |
organic matter | % | 6.62 |
particle density | g m−3 | 2.6 |
moisture content (dry basis) | % | 27.7 |
Wheel Type | Load Level | RMS Drawbar Pull, in N |
---|---|---|
standard tires | low | 518.056 |
high | 1274.652 | |
spike tires | low | 539.295 |
high | 1589.953 | |
blade wheels | low | 580.914 |
high | 3141.954 |
Wheel Type | Load Level | Tractor Speed, in m s−1 | Mean Drawbar Pull, in N | Standard Deviation, in N | Variation Coefficient, in % | Drawbar Power, in W |
---|---|---|---|---|---|---|
standard tires | low | 0.667 | 493.9 | 155.3 | 31.5 | 329.5 |
high | 0.306 | 1260.4 | 185.4 | 14.7 | 385.7 | |
spike tires | low | 0.731 | 513.4 | 164.1 | 31.9 | 375.4 |
high | 0.326 | 1578.3 | 184.9 | 11.7 | 514.5 | |
blade wheels | low | 0.751 | 530.5 | 236.1 | 49.6 | 398.4 |
high | 0.434 | 3129.4 | 261.4 | 8.4 | 1358.2 |
Wheel Type | Load | Rotation Speed of Driving Wheels, in s−1 | Model Frequency Interval | Experimental Frequency, in Hz | |
---|---|---|---|---|---|
Minimum Frequency, in Hz | Maximum Frequency, in Hz | ||||
standard tires | low | 0.41 | 6.56 | 13.12 | - |
high | - | ||||
spike tires | low | 1.64 | 3.28 | 3.27 | |
high | 3.13 | ||||
blade wheels | low | 4.09 | 8.18 | 4.11 | |
high | 3.91 |
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Abrahám, R.; Majdan, R.; Kollárová, K.; Tkáč, Z.; Olejár, M.; Matejková, E.; Kubík, Ľ. Frequency Spectra Analysis of Drawbar Pulls Generated by Special Driving Wheels Improving Tractive Performance. Sensors 2021, 21, 2903. https://doi.org/10.3390/s21092903
Abrahám R, Majdan R, Kollárová K, Tkáč Z, Olejár M, Matejková E, Kubík Ľ. Frequency Spectra Analysis of Drawbar Pulls Generated by Special Driving Wheels Improving Tractive Performance. Sensors. 2021; 21(9):2903. https://doi.org/10.3390/s21092903
Chicago/Turabian StyleAbrahám, Rudolf, Radoslav Majdan, Katarína Kollárová, Zdenko Tkáč, Martin Olejár, Eva Matejková, and Ľubomír Kubík. 2021. "Frequency Spectra Analysis of Drawbar Pulls Generated by Special Driving Wheels Improving Tractive Performance" Sensors 21, no. 9: 2903. https://doi.org/10.3390/s21092903
APA StyleAbrahám, R., Majdan, R., Kollárová, K., Tkáč, Z., Olejár, M., Matejková, E., & Kubík, Ľ. (2021). Frequency Spectra Analysis of Drawbar Pulls Generated by Special Driving Wheels Improving Tractive Performance. Sensors, 21(9), 2903. https://doi.org/10.3390/s21092903